The dynamical behaviour of the I-E polarization curves of the Co 1 M H 3PO 4 electrochemical oscillator is studied as the potential varies across the active/passive transition of the Co electrode. An oscillatory potential region exists between the two stable steady-states where a hysteresis loop is formed by the sudden decrease (Co passivation) and increase (Co activation) of the current as the potential is scanned forward and backward. In the present study an attempt is made towards an experimental determination of the bifurcation structure of the Co 1 M H 3PO 4 system. Transition from the active steadystate (SS1) to the oscillatory state (OSC), and vice versa, is accompanied by a hysteresis and occurs at critical potential values via a generalised Hopf bifurcation. The identification of the generalised Hopf bifurcation is based on the presence of hysteresis, the sudden appearance of full amplitude oscillations during the transition SS1 → OSC and on the fact that the transition OSC → SS1 occurs with oscillations of a finite amplitude. On the other side of the loop, transition from the oscillatory region to the passive steady-state (SS2) goes via a saddle-type bifurcation. The period lengthening during the transition OSC → SS2, the existence of small hysteresis and the fact that oscillations appear and disappear with almost their full amplitude ensure a saddle-type bifurcation. Some of the bifurcation features are discussed on the basis of the surface processes taking place at the Co electrode and compared with the Fe 2 M H 2SO 4 electrochemical oscillator that was previously investigated. Potential and current perturbation experiments applied close to bifurcation points indicate that the Co 1 M H 3PO 4 system does not exhibit excitability in the corresponding regions where Fe 2 M H 2SO 4 does. Micrographs taken by the scanning electron microscope and examination of the chloride effect on the dynamical behaviour of the Co 1 M H 3PO 4 system support further the relation between the experimental findings and the mechanism leading to the non-linear behaviour across the active-passive transition.
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